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<front>
<journal-meta>
<journal-id journal-id-type="pmc">CMES</journal-id>
<journal-id journal-id-type="nlm-ta">CMES</journal-id>
<journal-id journal-id-type="publisher-id">CMES</journal-id>
<journal-title-group>
<journal-title>Computer Modeling in Engineering &#x0026; Sciences</journal-title>
</journal-title-group>
<issn pub-type="epub">1526-1506</issn>
<issn pub-type="ppub">1526-1492</issn>
<publisher>
<publisher-name>Tech Science Press</publisher-name>
<publisher-loc>USA</publisher-loc>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">55679</article-id>
<article-id pub-id-type="doi">10.32604/cmes.2024.055679</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Article</subject>
</subj-group>
</article-categories>
<title-group>
<article-title>Performance Analysis of Curved Track G2T-FSO (Ground-to-Train Free Space Optical) Model under Various Weather Conditions</article-title>
<alt-title alt-title-type="left-running-head">Performance Analysis of Curved Track G2T-FSO (Ground-to-Train Free Space Optical) Model under Various Weather Conditions</alt-title>
<alt-title alt-title-type="right-running-head">Performance Analysis of Curved Track G2T-FSO (Ground-to-Train Free Space Optical) Model under Various Weather Conditions</alt-title>
</title-group>
<contrib-group>
<contrib id="author-1" contrib-type="author" corresp="yes">
<name name-style="western"><surname>Alhartomi</surname><given-names>Mohammed A.</given-names></name><xref ref-type="aff" rid="aff-1">1</xref><email>malhartomi@ut.edu.sa</email></contrib>
<contrib id="author-2" contrib-type="author">
<name name-style="western"><surname>Abdullah</surname><given-names>Mohammad F. L.</given-names></name><xref ref-type="aff" rid="aff-2">2</xref></contrib>
<contrib id="author-3" contrib-type="author">
<name name-style="western"><surname>Mabrouk</surname><given-names>Wafi A. B.</given-names></name><xref ref-type="aff" rid="aff-2">2</xref></contrib>
<contrib id="author-4" contrib-type="author">
<name name-style="western"><surname>Gismalla</surname><given-names>Mohammed S. M.</given-names></name><xref ref-type="aff" rid="aff-3">3</xref></contrib>
<contrib id="author-5" contrib-type="author">
<name name-style="western"><surname>Alzahmi</surname><given-names>Ahmed</given-names></name><xref ref-type="aff" rid="aff-1">1</xref></contrib>
<contrib id="author-6" contrib-type="author">
<name name-style="western"><surname>Alzahrani</surname><given-names>Saeed</given-names></name><xref ref-type="aff" rid="aff-1">1</xref></contrib>
<contrib id="author-7" contrib-type="author">
<name name-style="western"><surname>Altimania</surname><given-names>Mohammad R.</given-names></name><xref ref-type="aff" rid="aff-1">1</xref></contrib>
<contrib id="author-8" contrib-type="author">
<name name-style="western"><surname>Alsawat</surname><given-names>Mohammed S.</given-names></name><xref ref-type="aff" rid="aff-4">4</xref></contrib>
<aff id="aff-1"><label>1</label><institution>Department of Electrical Engineering, University of Tabuk</institution>, <addr-line>Tabuk, 71491</addr-line>, <country>Saudi Arabia</country></aff>
<aff id="aff-2"><label>2</label><institution>Faculty of Electrical and Electronic Engineering, Universiti Tun Hussein Onn Malaysia (UTHM)</institution>, <addr-line>Johor, 86400</addr-line>, <country>Malaysia</country></aff>
<aff id="aff-3"><label>3</label><institution>Center for Communication Systems and Sensing, King Fahd University of Petroleum and Minerals (KFUPM)</institution>, <addr-line>Dhahran, 31261</addr-line>, <country>Saudi Arabia</country></aff>
<aff id="aff-4"><label>4</label><institution>Department of Mechanical Engineering, University of Tabuk</institution>, <addr-line>Tabuk, 71491</addr-line>, <country>Saudi Arabia</country></aff>
</contrib-group>
<author-notes>
<corresp id="cor1"><label>&#x002A;</label>Corresponding Author: Mohammed A. Alhartomi. Email: <email>malhartomi@ut.edu.sa</email></corresp>
</author-notes>
<pub-date date-type="collection" publication-format="electronic">
<year>2024</year></pub-date>
<pub-date date-type="pub" publication-format="electronic">
<day>31</day>
<month>10</month>
<year>2024</year>
</pub-date>
<volume>141</volume>
<issue>3</issue>
<fpage>2087</fpage>
<lpage>2105</lpage>
<history>
<date date-type="received">
<day>04</day>
<month>7</month>
<year>2024</year>
</date>
<date date-type="accepted">
<day>03</day>
<month>9</month>
<year>2024</year>
</date>
</history>
<permissions>
<copyright-statement>&#x00A9; 2024 The Authors.</copyright-statement>
<copyright-year>2024</copyright-year>
<copyright-holder>Published by Tech Science Press.</copyright-holder>
<license xlink:href="https://creativecommons.org/licenses/by/4.0/">
<license-p>This work is licensed under a <ext-link ext-link-type="uri" xlink:type="simple" xlink:href="https://creativecommons.org/licenses/by/4.0/">Creative Commons Attribution 4.0 International License</ext-link>, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.</license-p>
</license>
</permissions>
<self-uri content-type="pdf" xlink:href="TSP_CMES_55679.pdf"></self-uri>
<abstract>
<p>The demand for broadband data services on high-speed trains is rapidly growing as more people commute between their homes and workplaces. However, current radio frequency (RF) technology cannot adequately meet this demand. In order to address the bandwidth constraint, a technique known as free space optics (FSO) has been proposed. This paper presents a mathematical derivation and formulation of curve track G2T-FSO (Ground-to-train Free Space Optical) model, where the track radius characteristics is 2667 m, divergence angle track is 1.5&#x00B0; for train velocity at V &#x003D; 250 km/h. Multiple transmitter configurations are proposed to maximize coverage range and enhance curve track G2T-FSO link performance under varying weather conditions. The curved track G2T-FSO model was evaluated in terms of received power, signal-to-noise ratio (SNR), bit error rate (BER), and eye diagrams. The results showed maximum coverage lengths of 618, 505, 365, and 240 m for 4Tx/1Rx, 3Tx/1Rx, 2Tx/1Rx, and 1Tx/1Rx configurations, respectively. The analyzed results demonstrate that the G2T-FSO link can be effectively implemented under various weather conditions.</p>
</abstract>
<kwd-group kwd-group-type="author">
<kwd>Free space optics</kwd>
<kwd>curve track</kwd>
<kwd>ground-to-train communications</kwd>
<kwd>geometrical loss</kwd>
<kwd>weather conditions</kwd>
</kwd-group>
<funding-group>
<award-group id="awg1">
<funding-source>Deputyship for Research &#x0026; Innovation, Ministry of Education in Saudi Arabia</funding-source>
<award-id>S-1443-0223</award-id>
</award-group>
</funding-group>
</article-meta>
</front>
<body>
<sec id="s1">
<label>1</label>
<title>Introduction</title>
<p>With high-speed trains (HSTs) around the globe traveling at speeds over 250 km/h, they are increasingly favored for long-distance journeys. As the popularity of high-speed public transport and internet-connected devices grows, there is a rising demand for fast and reliable onboard internet. Current technologies, such as IEEE 802.11 p and Long-Term Evolution (LTE), can only meet certain requirements, especially at higher train speeds [<xref ref-type="bibr" rid="ref-1">1</xref>]. Even advanced radio frequency (RF) solutions, which theoretically offer speeds of 54/75 Mbps, often drop below 10 Mbps in real-world usage [<xref ref-type="bibr" rid="ref-2">2</xref>]. Free space optical (FSO) communication, also known as open-air photonics infrared broadband, uses light to transmit data through free space, including air, outer space, and vacuum. Operating in the 780&#x2013;1600 nm range, FSO achieves high data rates over distances from a few meters to a thousand kilometers, with applications in deep-space communications, unmanned vehicles, and ultra-high-speed trains. For high-speed trains exceeding 250 km/h, traditional RF technologies struggle to meet data demands due to challenges like the Doppler effect and frequent handovers [<xref ref-type="bibr" rid="ref-3">3</xref>,<xref ref-type="bibr" rid="ref-4">4</xref>]. The growing demand for swift connectivity on trains has boosted interest in ground-to-train (G2T) communication. The authors in [<xref ref-type="bibr" rid="ref-5">5</xref>,<xref ref-type="bibr" rid="ref-6">6</xref>] conducted an exploratory study on the feasibility of FSO systems in this context. Their findings revealed encouraging data transfer speeds, although the dynamics of a moving train introduced certain challenges. Authors in [<xref ref-type="bibr" rid="ref-1">1</xref>] introduced free-space optics technique for high-speed train communication that reduces the required number of base stations from 113 to fewer than 10 while achieving a fixed data rate of 1.25 Gbps, addressing limitations in existing technologies and accounting for various weather conditions. In [<xref ref-type="bibr" rid="ref-7">7</xref>], three wavelengths (850, 1330, and 1550 nm) in a dual-wavelength free-space optics model for high-speed train communication at a bit rate of 10 Gb/s.</p>
<p>There are various G2T-FSO models using numerical simulations that have been carried out utilizing various track geometry models and FSO performance evaluations. Paudel et al. [<xref ref-type="bibr" rid="ref-8">8</xref>] developed numerous models for G2T-FSO communication. The author developed a straight-track model based on a Lambertian model, with a light emitting diode (LED) assumed to establish the link. The geometrical models&#x2019; analysis obtained a 20 m range distance at 1 Gbps data rates. In addition, a curved track model with various geometrical features was developed in another work [<xref ref-type="bibr" rid="ref-9">9</xref>]. The expected turbulent loss, it provided coverage of 50 m at 100 Mbs and 154 m at 10 Mbps. It showed a limited track radius range of 120&#x2013;500 m, which does not allow for high-speed trains to operate on curves. Additionally, Reference [<xref ref-type="bibr" rid="ref-10">10</xref>] obtained data rates of 50 Mbps at link distances of 75 m using a Gaussian source model that leverages a laser diode for higher transmitted power. Several studies investigated the G2T-FSO straight-track concept, which obtained a variety of link ranges at varying data rates. Reference [<xref ref-type="bibr" rid="ref-11">11</xref>] obtained a coverage distance of 180 m at a high data rate of 5 Gbps, while Reference [<xref ref-type="bibr" rid="ref-3">3</xref>] optimized a model with two transceivers to attain 509 m coverage at 1 Gbps. Also, another model improved link performance to increase the 75 m range to 99 m at 1 Gbps [<xref ref-type="bibr" rid="ref-12">12</xref>]. Previous research investigated link coverage range, transceiver design, track configuration, bit error rate (BER), data rates, handover, number of base stations, and weather attenuation effects. Despite past work, current research frequently emphasizes straight-track configurations and the influence of a few parameters on FSO channel losses. Therefore, there is no adequate combination of weather attenuation effects, railway configuration, and FSO link configurations. Many attempts were made to extend coverage lengths; however, except in [<xref ref-type="bibr" rid="ref-5">5</xref>], it used a single-track FSO link with low data rate considerations. Mabrouk et al. [<xref ref-type="bibr" rid="ref-13">13</xref>] investigated the geometric loss in curved track G2T-FSO link and evaluated the impact of varying both vertical and horizontal distances. However, there is a shortage of comprehensive performance evaluation and performance improvement initiatives for curved track models.</p>
<p>Due to these shortcomings, further research was needed on G2T-FSO models, including multiple track geometries, performance enhancement, multiple base station (BS) transmitters, and weather conditions. This paper described the implementation of G2T-FSO communication links, utilizing the concept of multiple transmitters to achieve high-performance links with extended coverage ranges and improved data rates. It introduced new curved track G2T-FSO mathematical link model, accounting for driving speeds of up to 250 km/h, specifically considering high-speed train scenarios, which resulted in enhanced link performance. The evaluation of G2T-FSO link performance was characterized across various weather conditions, including clear, rainy, and foggy conditions, employing the NRZ modulation technique. The main contributions of this paper were as follows:
<list list-type="bullet">
<list-item>
<p>Derive a mathematical model for a curved track with clearance distance, FSO link, Cant excess, Cant deficit, and maximum radius. These values were chosen based on the train&#x2019;s physical characteristics and the maximum permitted speeds on a curve.</p></list-item>
<list-item>
<p>To Enhance G2T-FSO performance and expand link coverage ranges, we adopted the multi-transmitter concept and evaluated and depicted system performance in terms of received power, signal-to-noise ratio (SNR), BER, and eye diagram.</p></list-item>
</list></p>
<p>This paper is organized as follows: <xref ref-type="sec" rid="s2">Section 2</xref> presents the system model for curved track G2T-FSO communication, including the mathematical derivations. <xref ref-type="sec" rid="s3">Section 3</xref> provides the results, discussions, and performance evaluation of the G2T-FSO communication link. Finally, the paper concludes in <xref ref-type="sec" rid="s4">Section 4</xref>.</p>
</sec>
<sec id="s2">
<label>2</label>
<title>System Model</title>
<sec id="s2_1">
<label>2.1</label>
<title>Train Physical Behavior and Curved Track Alignment</title>
<p>This section discusses the factors influencing the position of a train on a curved railway, crucial for determining the appropriate track radius in developing the curved track G2T-FSO link model. Since the advent of railways in 1825, the basic systems for straight and curved track navigation have remained consistent. Unlike other vehicles, trains are guided by their wheelsets along the track without active steering by a driver [<xref ref-type="bibr" rid="ref-14">14</xref>]. On curved tracks, centrifugal forces cause the train to tilt. Key parameters include the cant angle (&#x03B4;-Cant), track cant (U), and track gauge (G), as shown in <xref ref-type="fig" rid="fig-1">Fig. 1</xref>. Residual lateral acceleration (&#x03B6;) is measured in m/s&#x00B2; or g, while cant excess (E) and cant deficiency (I) are measured in millimeters.</p>
<fig id="fig-1">
<label>Figure 1</label>
<caption>
<title>Position of the train in a curved track section</title>
</caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="CMES_55679-fig-1.tif"/>
</fig>
<p>In railway engineering, proper distribution of train load on wheelsets is essential, particularly on curved tracks with a specific cant (or superelevation). This design helps reduce wear and tear between the rails and rolling stock, counteracting the effects of lateral forces [<xref ref-type="bibr" rid="ref-15">15</xref>]. These measures ensure passenger comfort and prevent derailment by minimizing the risk of wheel slippage [<xref ref-type="bibr" rid="ref-16">16</xref>]. Additionally, trains must maintain an equilibrium speed when negotiating curves to balance train load forces and radial acceleration, keeping them perpendicular to the track plane. Cant helps counteract centrifugal forces at this equilibrium speed, ensuring stability and smooth operation [<xref ref-type="bibr" rid="ref-16">16</xref>].</p>
<p>Cant deficiency occurs when the train&#x2019;s speed exceeds the equilibrium speed, causing it to tilt towards the outer rail of the curve. Conversely, if the speed is lower than the equilibrium speed, cant deficiency causes the train to tilt towards the inner rail. To calculate the maximum permissible speed for a curve in this paper, parameters such as track cant length, cant excess, cant deficiency, and track radius must be considered. <xref ref-type="fig" rid="fig-2">Fig. 2</xref> illustrates the track curvature for a single wheelset, with <italic>V</italic> representing the train&#x2019;s speed along the curve [<xref ref-type="bibr" rid="ref-17">17</xref>].</p>
<fig id="fig-2">
<label>Figure 2</label>
<caption>
<title>Track curvature for the motion of a single wheelset</title>
</caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="CMES_55679-fig-2.tif"/>
</fig>
</sec>
<sec id="s2_2">
<label>2.2</label>
<title>Curved Track G2T-FSO Model with Considerations for Horizontal Alignment Radii</title>
<p><xref ref-type="fig" rid="fig-3">Fig. 3</xref> illustrates a curved track with G2T-FSO communication, where the link connects to ground base stations (BSs) along the railway. Multiple FSO transceivers on the train&#x2019;s roof enable line of sight (LOS) communication with the BSs. ZC1 is the propagation distance between the FSO transceiver and the BS, while <inline-formula id="ieqn-1"><mml:math id="mml-ieqn-1"><mml:msub><mml:mi>&#x03B8;</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> and <inline-formula id="ieqn-2"><mml:math id="mml-ieqn-2"><mml:msub><mml:mi>&#x03B8;</mml:mi><mml:mrow><mml:mrow><mml:mi>C</mml:mi><mml:msub><mml:mn>1</mml:mn><mml:mrow><mml:mfrac><mml:mn>1</mml:mn><mml:mn>2</mml:mn></mml:mfrac></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:msub></mml:math></inline-formula> represent the divergence and half-divergence angles, respectively.</p>
<fig id="fig-3">
<label>Figure 3</label>
<caption>
<title>Proposed G2T-FSO model for curved track</title>
</caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="CMES_55679-fig-3.tif"/>
</fig>
<p>The focus of this paper is on high-speed trains. They have no clear definition but are often recognized by driving speeds above 200 km/h [<xref ref-type="bibr" rid="ref-17">17</xref>,<xref ref-type="bibr" rid="ref-18">18</xref>]. Thus, the theoretical required horizontal radii to obtain high speeds might be determined by considering the physical behavior of trains over a curve. This can be achieved by considering the train&#x2019;s geometrical behavior in terms of maximum track deficiency as well as its physical behavior in terms of maximum permitted speeds along a horizontal alignment [<xref ref-type="bibr" rid="ref-19">19</xref>,<xref ref-type="bibr" rid="ref-20">20</xref>]. Assuming a speed of 250 km/h, the minimum required track radius to achieve this case might be approximated as [<xref ref-type="bibr" rid="ref-17">17</xref>]:
<disp-formula id="eqn-1"><label>(1)</label><mml:math id="mml-eqn-1" display="block"><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>11.8</mml:mn><mml:mspace width="thinmathspace" /><mml:msubsup><mml:mi>V</mml:mi><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup></mml:mrow><mml:mrow><mml:msub><mml:mi>U</mml:mi><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>I</mml:mi><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo stretchy="false">(</mml:mo><mml:mi>m</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:math></disp-formula>where <inline-formula id="ieqn-3"><mml:math id="mml-ieqn-3"><mml:msub><mml:mi>V</mml:mi><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>, <inline-formula id="ieqn-4"><mml:math id="mml-ieqn-4"><mml:msub><mml:mi>U</mml:mi><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>, and <inline-formula id="ieqn-5"><mml:math id="mml-ieqn-5"><mml:msub><mml:mi>I</mml:mi><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> are maximum permissible track speeds (km/h), track <italic>Cant</italic> (mm) and <italic>Cant deficiency</italic> (mm). In addition to the minimum curve radius in horizontal alignment is <inline-formula id="ieqn-6"><mml:math id="mml-ieqn-6"><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>m</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:math></inline-formula>. <inline-formula id="ieqn-7"><mml:math id="mml-ieqn-7"><mml:msub><mml:mi>I</mml:mi><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is calculated using <xref ref-type="disp-formula" rid="eqn-2">Eq. (2)</xref> [<xref ref-type="bibr" rid="ref-17">17</xref>,<xref ref-type="bibr" rid="ref-21">21</xref>]:
<disp-formula id="eqn-2"><label>(2)</label><mml:math id="mml-eqn-2" display="block"><mml:msub><mml:mi>I</mml:mi><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mi>G</mml:mi><mml:mi>a</mml:mi><mml:mi>g</mml:mi><mml:mi>e</mml:mi></mml:mrow><mml:mi>g</mml:mi></mml:mfrac><mml:msub><mml:mrow><mml:mi mathvariant="normal">&#x03B6;</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>m</mml:mi><mml:mi>m</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>,</mml:mo></mml:math></disp-formula>where <inline-formula id="ieqn-8"><mml:math id="mml-ieqn-8"><mml:msub><mml:mrow><mml:mi mathvariant="normal">&#x03B6;</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is the highest residual lateral acceleration in (m/s<sup>2</sup>), &#x201C;<italic>Gage</italic>&#x201D; is track gage, which is the distance among centers both rails, and <italic>g</italic> is the acceleration of gravity (m/s). It is preferable to have a design that ensures passenger comfort [<xref ref-type="bibr" rid="ref-16">16</xref>]. Hence, a lateral acceleration value of 0.5 was adopted, as it is recognized to have an inverse relationship with passenger comfort. The selection of these values was made based on the application of the Joly and Pyrgidis model, which addresses the lateral behavior of railway vehicles on curves [<xref ref-type="bibr" rid="ref-22">22</xref>&#x2013;<xref ref-type="bibr" rid="ref-24">24</xref>]. A typical value of 200 m was chosen for <inline-formula id="ieqn-9"><mml:math id="mml-ieqn-9"><mml:msub><mml:mi>U</mml:mi><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>. A curved track radius of 2667 m is obtained by substituting variable values in <xref ref-type="disp-formula" rid="eqn-1">Eq. (1)</xref>.</p>
</sec>
<sec id="s2_3">
<label>2.3</label>
<title>Geometrical Properties</title>
<p><xref ref-type="fig" rid="fig-4">Fig. 4</xref> illustrates the geometrical attributes of the G2T-FSO curved track on <italic>x</italic> and <italic>y</italic> axes. <italic>R</italic><sub><italic>C</italic></sub> denotes the track radius, and <inline-formula id="ieqn-10"><mml:math id="mml-ieqn-10"><mml:msub><mml:mi>&#x03D6;</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> is the angle between <inline-formula id="ieqn-11"><mml:math id="mml-ieqn-11"><mml:mi>T</mml:mi><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>C</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> and <inline-formula id="ieqn-12"><mml:math id="mml-ieqn-12"><mml:mi>R</mml:mi><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>C</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> [<xref ref-type="bibr" rid="ref-9">9</xref>]. The FSO LOS is established between the BS and the train transceiver at <inline-formula id="ieqn-13"><mml:math id="mml-ieqn-13"><mml:mi>T</mml:mi><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>C</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> and <inline-formula id="ieqn-14"><mml:math id="mml-ieqn-14"><mml:mi>R</mml:mi><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>C</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>. The BS positioned is set with a horizontal distance <inline-formula id="ieqn-15"><mml:math id="mml-ieqn-15"><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mrow><mml:msub><mml:mi>H</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:msub></mml:math></inline-formula> and vertical distance <inline-formula id="ieqn-16"><mml:math id="mml-ieqn-16"><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mrow><mml:msub><mml:mi>V</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:msub></mml:math></inline-formula> from the track. <inline-formula id="ieqn-17"><mml:math id="mml-ieqn-17"><mml:mi>&#x03C6;</mml:mi></mml:math></inline-formula> is irradiance angle, <inline-formula id="ieqn-18"><mml:math id="mml-ieqn-18"><mml:mi>&#x03C8;</mml:mi></mml:math></inline-formula> is the incident angle at <inline-formula id="ieqn-19"><mml:math id="mml-ieqn-19"><mml:mi>R</mml:mi><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>C</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> and <inline-formula id="ieqn-20"><mml:math id="mml-ieqn-20"><mml:mi>&#x03B3;</mml:mi></mml:math></inline-formula> is the tilting angle.</p>
<fig id="fig-4">
<label>Figure 4</label>
<caption>
<title>Geometrical properties and LOS considerations of curved track G2T-FSO link</title>
</caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="CMES_55679-fig-4.tif"/>
</fig>
<p>The parameter &#x03B4; represents the coverage angle along the propagation distance <inline-formula id="ieqn-21"><mml:math id="mml-ieqn-21"><mml:msub><mml:mi>Z</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> between the beam edge and <italic>x</italic>-axis. Defining <inline-formula id="ieqn-22"><mml:math id="mml-ieqn-22"><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> and <inline-formula id="ieqn-23"><mml:math id="mml-ieqn-23"><mml:msub><mml:mi>Q</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> as <italic>x</italic> and <italic>y</italic> coordinates, the divergence angle <inline-formula id="ieqn-24"><mml:math id="mml-ieqn-24"><mml:msub><mml:mi>&#x03B8;</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> can be determined. Additionally, &#x03B2; and &#x03B4; represent the coverage angles for <inline-formula id="ieqn-25"><mml:math id="mml-ieqn-25"><mml:mi>T</mml:mi><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> and <inline-formula id="ieqn-26"><mml:math id="mml-ieqn-26"><mml:mi>R</mml:mi><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> at the short and long ends, respectively.</p>
<p>According to <xref ref-type="fig" rid="fig-4">Fig. 4</xref>, the angle between <inline-formula id="ieqn-27"><mml:math id="mml-ieqn-27"><mml:mi>T</mml:mi><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> and <inline-formula id="ieqn-28"><mml:math id="mml-ieqn-28"><mml:mi>R</mml:mi><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula>, which is denoted as <inline-formula id="ieqn-29"><mml:math id="mml-ieqn-29"><mml:msub><mml:mi>&#x03D6;</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> is expressed as:
<disp-formula id="eqn-3"><label>(3)</label><mml:math id="mml-eqn-3" display="block"><mml:msub><mml:mi>&#x03D6;</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mrow><mml:msub><mml:mi>H</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mfrac><mml:mo>,</mml:mo></mml:math></disp-formula>where <inline-formula id="ieqn-30"><mml:math id="mml-ieqn-30"><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> is curve radius, <inline-formula id="ieqn-31"><mml:math id="mml-ieqn-31"><mml:mi>&#x03C6;</mml:mi></mml:math></inline-formula> and <inline-formula id="ieqn-32"><mml:math id="mml-ieqn-32"><mml:mi>&#x03C8;</mml:mi></mml:math></inline-formula> represent the irradiance and incident angles, respectively, and <inline-formula id="ieqn-33"><mml:math id="mml-ieqn-33"><mml:mi>&#x03B3;</mml:mi></mml:math></inline-formula> is tilting angle, defined as:
<disp-formula id="eqn-4"><label>(4)</label><mml:math id="mml-eqn-4" display="block"><mml:mi>&#x03B3;</mml:mi><mml:mo>=</mml:mo><mml:mfrac><mml:msub><mml:mi>&#x03B8;</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mn>2</mml:mn></mml:mfrac><mml:mo>+</mml:mo><mml:mi>&#x03B4;</mml:mi><mml:mo>.</mml:mo></mml:math></disp-formula></p>
<p>The angle between the beam edge and <italic>x</italic>-axis is &#x03B4;, which is defined as:
<disp-formula id="eqn-5"><label>(5)</label><mml:math id="mml-eqn-5" display="block"><mml:mi>&#x03B4;</mml:mi><mml:mo>=</mml:mo><mml:msup><mml:mi>tan</mml:mi><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msup><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mfrac><mml:msub><mml:mi>Q</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mfrac><mml:mo>)</mml:mo></mml:mrow><mml:mo>.</mml:mo></mml:math></disp-formula></p>
<p>Given Q<sub>C1</sub> <italic>y</italic>-axis coordinate, P<sub>C1</sub> <italic>x</italic>-axis coordinate might be defined as:
<disp-formula id="eqn-6"><label>(6)</label><mml:math id="mml-eqn-6" display="block"><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>&#x22C5;</mml:mo><mml:mo stretchy="false">(</mml:mo><mml:mi>s</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:msub><mml:mi>&#x03D6;</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">)</mml:mo><mml:mo stretchy="false">)</mml:mo></mml:math></disp-formula></p>
<p>Using Pythagorean theorem
<disp-formula id="eqn-7"><label>(7)</label><mml:math id="mml-eqn-7" display="block"><mml:msqrt><mml:msup><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mo>&#x2212;</mml:mo><mml:msup><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:msqrt><mml:mo>=</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>V</mml:mi><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>Q</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo></mml:math></disp-formula>which indicates that,
<disp-formula id="eqn-8"><label>(8)</label><mml:math id="mml-eqn-8" display="block"><mml:msub><mml:mi>Q</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msqrt><mml:msup><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mo>&#x2212;</mml:mo><mml:msup><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:msqrt><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>V</mml:mi><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>.</mml:mo></mml:math></disp-formula></p>
<p>Assuming the curved track divergence angle,
<disp-formula id="eqn-9"><label>(9)</label><mml:math id="mml-eqn-9" display="block"><mml:msub><mml:mi>&#x03B8;</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mi>&#x03B2;</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mi>&#x03B4;</mml:mi><mml:mo>.</mml:mo></mml:math></disp-formula></p>
<p>Given that,
<disp-formula id="eqn-10"><label>(10)</label><mml:math id="mml-eqn-10" display="block"><mml:mi>&#x03B2;</mml:mi><mml:mo>=</mml:mo><mml:msup><mml:mi>tan</mml:mi><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msup><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mfrac><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>V</mml:mi><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>H</mml:mi><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mfrac><mml:mo>)</mml:mo></mml:mrow><mml:mo>.</mml:mo></mml:math></disp-formula></p>
<p>Further, the receiver&#x2019;s irradiance angle is:
<disp-formula id="eqn-11"><label>(11)</label><mml:math id="mml-eqn-11" display="block"><mml:mi>&#x03B4;</mml:mi><mml:mo>=</mml:mo><mml:msup><mml:mi>tan</mml:mi><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msup><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mfrac><mml:msub><mml:mi>Q</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mfrac><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula></p>
<p>Therefore, the divergence angle for the first curved track <inline-formula id="ieqn-34"><mml:math id="mml-ieqn-34"><mml:msub><mml:mi>&#x03B8;</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> is defined as:
<disp-formula id="eqn-12"><label>(12)</label><mml:math id="mml-eqn-12" display="block"><mml:msub><mml:mi>&#x03B8;</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mi>t</mml:mi><mml:mi>a</mml:mi><mml:msup><mml:mi>n</mml:mi><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mfrac><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>V</mml:mi><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>H</mml:mi><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mfrac><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mi>t</mml:mi><mml:mi>a</mml:mi><mml:msup><mml:mi>n</mml:mi><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mfrac><mml:msub><mml:mi>Q</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mfrac><mml:mo>)</mml:mo></mml:mrow><mml:mo>.</mml:mo></mml:math></disp-formula></p>
<p>However, the propagation length is formulated as:
<disp-formula id="eqn-13"><label>(13)</label><mml:math id="mml-eqn-13" display="block"><mml:msub><mml:mi>Z</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msqrt><mml:msup><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mo stretchy="false">(</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">)</mml:mo><mml:mo>+</mml:mo><mml:msup><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mo stretchy="false">(</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">)</mml:mo></mml:msqrt></mml:math></disp-formula></p>
<p>In an FSO link with a clear LOS, side clearance is needed. Referring to <xref ref-type="fig" rid="fig-3">Fig. 3</xref> for clearances beside the curved track, where <inline-formula id="ieqn-35"><mml:math id="mml-ieqn-35"><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> is the arc length with <inline-formula id="ieqn-36"><mml:math id="mml-ieqn-36"><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> radius. Given that <inline-formula id="ieqn-37"><mml:math id="mml-ieqn-37"><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mrow><mml:mo>/</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:math></inline-formula> is half arc length, the Sagitta of the curved track arc is <inline-formula id="ieqn-38"><mml:math id="mml-ieqn-38"><mml:msub><mml:mi>S</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula>. <inline-formula id="ieqn-39"><mml:math id="mml-ieqn-39"><mml:msubsup><mml:mi>S</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2032;</mml:mi></mml:mrow></mml:msubsup></mml:math></inline-formula> shows the minimal obstacle-free LOS as half Sagitta. The Sagitta of a circular arc that depicts rail track curve is used to assess track side clearance for LOS to FSO link:
<disp-formula id="eqn-14"><label>(14)</label><mml:math id="mml-eqn-14" display="block"><mml:msub><mml:mi>S</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msubsup><mml:mi>S</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2032;</mml:mi></mml:mrow></mml:msubsup><mml:mo>+</mml:mo><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>V</mml:mi><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></disp-formula>and since
<disp-formula id="eqn-15"><label>(15)</label><mml:math id="mml-eqn-15" display="block"><mml:msubsup><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2032;</mml:mi></mml:mrow></mml:msubsup><mml:mo>=</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>V</mml:mi><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>.</mml:mo></mml:math></disp-formula></p>
<p>Thus, the length of <italic>C</italic><sub><italic>C</italic>1</sub> of arch within radius <italic>R</italic><sub><italic>C</italic>1</sub> is defined as:
<disp-formula id="eqn-16"><label>(16)</label><mml:math id="mml-eqn-16" display="block"><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn>2</mml:mn><mml:mo stretchy="false">(</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mrow><mml:msub><mml:mi>V</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:msub><mml:mo stretchy="false">)</mml:mo><mml:mi>s</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>&#x03B4;</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>.</mml:mo></mml:math></disp-formula></p>
<p>As shown in <xref ref-type="fig" rid="fig-3">Fig. 3</xref>, Sagitta <inline-formula id="ieqn-40"><mml:math id="mml-ieqn-40"><mml:msub><mml:mi>S</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> length is the minimum obstacle-free distance for railway track to provide reliable LOS.
<disp-formula id="eqn-17"><label>(17)</label><mml:math id="mml-eqn-17" display="block"><mml:msubsup><mml:mi>S</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2032;</mml:mi></mml:mrow></mml:msubsup><mml:mo>=</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>&#x2212;</mml:mo><mml:msqrt><mml:msubsup><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup><mml:mo>&#x2212;</mml:mo><mml:mfrac><mml:msubsup><mml:mi>C</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup><mml:mn>4</mml:mn></mml:mfrac></mml:msqrt><mml:mo>=</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>&#x2212;</mml:mo><mml:msqrt><mml:msubsup><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup><mml:mo>&#x2212;</mml:mo><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>&#x22C5;</mml:mo><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>V</mml:mi><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mi>s</mml:mi><mml:mi>i</mml:mi><mml:msup><mml:mi>n</mml:mi><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mi>&#x03B4;</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msqrt><mml:mo>.</mml:mo></mml:math></disp-formula></p>
<p>Considering a non-diffraction limited geometrical loss, which is a function of divergence angle <inline-formula id="ieqn-41"><mml:math id="mml-ieqn-41"><mml:mi>&#x03B8;</mml:mi></mml:math></inline-formula> and link <inline-formula id="ieqn-42"><mml:math id="mml-ieqn-42"><mml:mi>Z</mml:mi></mml:math></inline-formula> range defined as [<xref ref-type="bibr" rid="ref-2">2</xref>]:
<disp-formula id="eqn-18"><label>(18)</label><mml:math id="mml-eqn-18" display="block"><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>G</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>s</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>d</mml:mi><mml:mi>B</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>=</mml:mo><mml:mn>20</mml:mn><mml:mo>&#x2217;</mml:mo><mml:msub><mml:mi>log</mml:mi><mml:mrow><mml:mn>10</mml:mn></mml:mrow></mml:msub><mml:mo>&#x2061;</mml:mo><mml:msup><mml:mrow><mml:mo>{</mml:mo><mml:mfrac><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>R</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>m</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msub><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>T</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>m</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mo stretchy="false">(</mml:mo><mml:msub><mml:mi>Z</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mi>m</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msub><mml:mo>&#x2217;</mml:mo><mml:msub><mml:mi>&#x03B8;</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>m</mml:mi><mml:mi>r</mml:mi><mml:mi>a</mml:mi><mml:mi>d</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msub><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mfrac><mml:mo>}</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mrow><mml:mtext>dB</mml:mtext></mml:mrow><mml:mo>,</mml:mo></mml:math></disp-formula>where d<sub><italic>R</italic></sub> is the receiver aperture diameter, <italic>d</italic><sub><italic>T</italic></sub> is the transmitter aperture diameter, <italic>Z is</italic> the LOS range in km, and <italic>L</italic><sub><italic>G (dB)</italic></sub> represents the specific geometrical loss in disciples.</p>
<p>Referring to <xref ref-type="disp-formula" rid="eqn-18">Eq. (18)</xref>, and substituting <xref ref-type="disp-formula" rid="eqn-7">Eqs. (7)</xref> and <xref ref-type="disp-formula" rid="eqn-8">(8)</xref> into <xref ref-type="disp-formula" rid="eqn-18">(18)</xref> geometrical loss at curve track is defined as:
<disp-formula id="eqn-19"><label>(19)</label><mml:math id="mml-eqn-19" display="block"><mml:mtable columnalign="left" rowspacing="3pt" columnspacing="0em 2em 0em 2em 0em 2em 0em 2em 0em 2em 0em" displaystyle="true"><mml:mtr><mml:mtd><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>G</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>C</mml:mi><mml:mn>1</mml:mn><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mi>d</mml:mi><mml:mi>B</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn>20</mml:mn><mml:msub><mml:mi>log</mml:mi><mml:mrow><mml:mn>10</mml:mn></mml:mrow></mml:msub><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:mo>[</mml:mo><mml:mfrac><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>g</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:msqrt><mml:msup><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>+</mml:mo><mml:msup><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:msqrt><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2217;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:msup><mml:mi>tan</mml:mi><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msup><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mfrac><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>V</mml:mi><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>H</mml:mi><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mfrac></mml:mstyle><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:msup><mml:mi>tan</mml:mi><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msup><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mfrac><mml:msqrt><mml:msup><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mi>sin</mml:mi><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>&#x03D6;</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>V</mml:mi><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:msqrt><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>&#x22C5;</mml:mo><mml:mi>sin</mml:mi><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>&#x03D6;</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>.</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>)</mml:mo></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:mfrac><mml:mo>]</mml:mo></mml:mrow><mml:mspace width="negativethinmathspace" /><mml:mo>.</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula></p>
</sec>
<sec id="s2_4">
<label>2.4</label>
<title>Received Power</title>
<p>The optical received power of a single FSO transmitter is typically defined as [<xref ref-type="bibr" rid="ref-25">25</xref>]:
<disp-formula id="eqn-20"><label>(20)</label><mml:math id="mml-eqn-20" display="block"><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>R</mml:mi><mml:mi>e</mml:mi><mml:mi>c</mml:mi><mml:mi>e</mml:mi><mml:mi>i</mml:mi><mml:mi>v</mml:mi><mml:mi>e</mml:mi><mml:mi>d</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mn>7</mml:mn></mml:mrow></mml:msub><mml:mo>&#x00D7;</mml:mo><mml:mfrac><mml:msubsup><mml:mi>d</mml:mi><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mi>&#x03B8;</mml:mi><mml:mo>&#x22C5;</mml:mo><mml:mi>Z</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mfrac><mml:mo>&#x00D7;</mml:mo><mml:msup><mml:mn>10</mml:mn><mml:mrow><mml:mfrac><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mi>&#x03B1;</mml:mi><mml:mi>Z</mml:mi></mml:mrow><mml:mn>10</mml:mn></mml:mfrac></mml:mrow></mml:msup><mml:mo>.</mml:mo></mml:math></disp-formula></p>
<p><inline-formula id="ieqn-43"><mml:math id="mml-ieqn-43"><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>R</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>, <inline-formula id="ieqn-44"><mml:math id="mml-ieqn-44"><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>, and <inline-formula id="ieqn-45"><mml:math id="mml-ieqn-45"><mml:mi>Z</mml:mi></mml:math></inline-formula> are the receiver and transmitter aperture diameters (m), and LOS range in km, respectively. PT and denote to the transmitter power and atmospheric attenuation factor (dB/Km), respectively. Substitute <xref ref-type="disp-formula" rid="eqn-13">Eqs. (13)</xref> and <xref ref-type="disp-formula" rid="eqn-14">(14)</xref> into <xref ref-type="disp-formula" rid="eqn-20">(20)</xref>, the derived received power for curved track G2T-FSO link is defined in <xref ref-type="disp-formula" rid="eqn-20">(20)</xref>. It is further defined in terms of geometrical properties as by substituting <xref ref-type="disp-formula" rid="eqn-6">Eqs. (6)</xref> and <xref ref-type="disp-formula" rid="eqn-8">(8)</xref> into <xref ref-type="disp-formula" rid="eqn-20">(20)</xref> as displayed in <xref ref-type="disp-formula" rid="eqn-21">(21)</xref>.
<disp-formula id="eqn-21"><label>(21)</label><mml:math id="mml-eqn-21" display="block"><mml:mtable columnalign="right left right left right left right left right left right left" rowspacing="3pt" columnspacing="0em 2em 0em 2em 0em 2em 0em 2em 0em 2em 0em" displaystyle="true"><mml:mtr><mml:mtd><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>R</mml:mi><mml:mi>e</mml:mi><mml:mi>c</mml:mi><mml:mi>e</mml:mi><mml:mi>i</mml:mi><mml:mi>v</mml:mi><mml:mi>e</mml:mi><mml:mi>d</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>C</mml:mi><mml:mn>1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub></mml:mtd><mml:mtd><mml:mi></mml:mi><mml:mo>=</mml:mo></mml:mtd></mml:mtr><mml:mtr><mml:mtd /><mml:mtd><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:msub><mml:mo>&#x00D7;</mml:mo><mml:mfrac><mml:msubsup><mml:mi>d</mml:mi><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mfrac><mml:mrow><mml:msup><mml:mi>tan</mml:mi><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msup><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mfrac><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>V</mml:mi><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>H</mml:mi><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mfrac></mml:mstyle><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:msup><mml:mi>tan</mml:mi><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msup><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mfrac><mml:mrow><mml:msqrt><mml:msup><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mo>&#x2212;</mml:mo><mml:msup><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:msqrt><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>V</mml:mi><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>&#x22C5;</mml:mo><mml:mi>sin</mml:mi><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>&#x03D6;</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>)</mml:mo></mml:mrow></mml:mrow><mml:mn>2</mml:mn></mml:mfrac></mml:mstyle><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:msqrt><mml:msup><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>+</mml:mo><mml:msup><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:msqrt><mml:mo>)</mml:mo></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mfrac><mml:mo>&#x00D7;</mml:mo><mml:msup><mml:mn>10</mml:mn><mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mfrac><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mi>&#x03B1;</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msqrt><mml:msup><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>+</mml:mo><mml:msup><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>.</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:msqrt><mml:mo>)</mml:mo></mml:mrow></mml:mrow><mml:mn>10</mml:mn></mml:mfrac><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msup><mml:mspace width="negativethinmathspace" /><mml:mo>.</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula></p>
</sec>
<sec id="s2_5">
<label>2.5</label>
<title>Receiver Performance Evaluation</title>
<p>The received power at the receiver for a single transmitter depends on the lens aperture diameter <inline-formula id="ieqn-46"><mml:math id="mml-ieqn-46"><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>T</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>m</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msub></mml:math></inline-formula>, transmitter aperture diameter <inline-formula id="ieqn-47"><mml:math id="mml-ieqn-47"><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>R</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>m</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msub></mml:math></inline-formula>, channel attenuation factor <inline-formula id="ieqn-48"><mml:math id="mml-ieqn-48"><mml:mi>&#x03B1;</mml:mi></mml:math></inline-formula> (dB/km), link range <inline-formula id="ieqn-49"><mml:math id="mml-ieqn-49"><mml:mi>Z</mml:mi></mml:math></inline-formula> (km), and divergence angle <inline-formula id="ieqn-50"><mml:math id="mml-ieqn-50"><mml:mi>&#x03B8;</mml:mi></mml:math></inline-formula> (mrad). The equation is given as [<xref ref-type="bibr" rid="ref-25">25</xref>]:
<disp-formula id="eqn-22"><label>(22)</label><mml:math id="mml-eqn-22" display="block"><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>R</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>T</mml:mi><mml:mi>o</mml:mi><mml:mi>t</mml:mi><mml:mi>a</mml:mi><mml:mi>l</mml:mi></mml:mrow></mml:msub><mml:mo>&#x2217;</mml:mo><mml:mfrac><mml:msubsup><mml:mi>d</mml:mi><mml:mrow><mml:mi>R</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>m</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup><mml:msup><mml:mrow><mml:mo>[</mml:mo><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>T</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>m</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mi>&#x03B8;</mml:mi><mml:mo>&#x2217;</mml:mo><mml:msub><mml:mi>Z</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mi>m</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mfrac><mml:mo>&#x2217;</mml:mo><mml:msup><mml:mn>10</mml:mn><mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mo>&#x2212;</mml:mo><mml:mi>&#x03B1;</mml:mi><mml:mo>&#x2217;</mml:mo><mml:mfrac><mml:msub><mml:mi>Z</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mi>m</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msub><mml:mn>10</mml:mn></mml:mfrac><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msup><mml:mo>.</mml:mo></mml:math></disp-formula></p>
<p>The photodetector converts the optical signal to an electrical signal. During detection, the signal faces various noise sources: shot noise <inline-formula id="ieqn-51"><mml:math id="mml-ieqn-51"><mml:msubsup><mml:mi>&#x03C3;</mml:mi><mml:mrow><mml:mi>S</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>t</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup></mml:math></inline-formula>, thermal noise <inline-formula id="ieqn-52"><mml:math id="mml-ieqn-52"><mml:msubsup><mml:mi>&#x03C3;</mml:mi><mml:mrow><mml:mi>T</mml:mi><mml:mi>h</mml:mi><mml:mi>e</mml:mi><mml:mi>r</mml:mi><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>l</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup></mml:math></inline-formula>, and background noise <inline-formula id="ieqn-53"><mml:math id="mml-ieqn-53"><mml:msubsup><mml:mi>&#x03C3;</mml:mi><mml:mrow><mml:mi>B</mml:mi><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mi>k</mml:mi><mml:mi>g</mml:mi><mml:mi>r</mml:mi><mml:mi>o</mml:mi><mml:mi>u</mml:mi><mml:mi>n</mml:mi><mml:mi>d</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup></mml:math></inline-formula>. These are used to calculate the SNR as defined by [<xref ref-type="bibr" rid="ref-26">26</xref>,<xref ref-type="bibr" rid="ref-27">27</xref>]:
<disp-formula id="eqn-23"><label>(23)</label><mml:math id="mml-eqn-23" display="block"><mml:mi>S</mml:mi><mml:mi>N</mml:mi><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi mathvariant="fraktur">R</mml:mi></mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>R</mml:mi><mml:mi>e</mml:mi><mml:mi>c</mml:mi><mml:mi>e</mml:mi><mml:mi>i</mml:mi><mml:mi>v</mml:mi><mml:mi>e</mml:mi><mml:mi>d</mml:mi></mml:mrow></mml:msub><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:msubsup><mml:mi>&#x03C3;</mml:mi><mml:mrow><mml:mi>T</mml:mi><mml:mi>o</mml:mi><mml:mi>t</mml:mi><mml:mi>a</mml:mi><mml:mi>l</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup></mml:mfrac><mml:mo>,</mml:mo></mml:math></disp-formula>where
<disp-formula id="eqn-24"><label>(24)</label><mml:math id="mml-eqn-24" display="block"><mml:msub><mml:mi>&#x03C3;</mml:mi><mml:mrow><mml:mi>T</mml:mi><mml:mi>o</mml:mi><mml:mi>t</mml:mi><mml:mi>a</mml:mi><mml:mi>l</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msubsup><mml:mi>&#x03C3;</mml:mi><mml:mrow><mml:mi>S</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>t</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi>&#x03C3;</mml:mi><mml:mrow><mml:mi>T</mml:mi><mml:mi>h</mml:mi><mml:mi>e</mml:mi><mml:mi>r</mml:mi><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>l</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi>&#x03C3;</mml:mi><mml:mrow><mml:mi>B</mml:mi><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mi>k</mml:mi><mml:mi>g</mml:mi><mml:mi>r</mml:mi><mml:mi>o</mml:mi><mml:mi>u</mml:mi><mml:mi>n</mml:mi><mml:mi>d</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup><mml:mo>,</mml:mo></mml:math></disp-formula>
<disp-formula id="eqn-25"><label>(25)</label><mml:math id="mml-eqn-25" display="block"><mml:msubsup><mml:mi>&#x03C3;</mml:mi><mml:mrow><mml:mi>T</mml:mi><mml:mi>h</mml:mi><mml:mi>e</mml:mi><mml:mi>r</mml:mi><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>l</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup><mml:mo>=</mml:mo><mml:mrow><mml:mo>&#x27E8;</mml:mo><mml:msubsup><mml:mi>i</mml:mi><mml:mrow><mml:mi>T</mml:mi><mml:mi>h</mml:mi><mml:mi>e</mml:mi><mml:mi>r</mml:mi><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>l</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup><mml:mo>&#x27E9;</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>4</mml:mn><mml:msub><mml:mi>K</mml:mi><mml:mrow><mml:mi>B</mml:mi></mml:mrow></mml:msub><mml:mi>T</mml:mi><mml:mi>B</mml:mi></mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>L</mml:mi></mml:mrow></mml:msub></mml:mfrac><mml:mo>,</mml:mo></mml:math></disp-formula>
<disp-formula id="eqn-26"><label>(26)</label><mml:math id="mml-eqn-26" display="block"><mml:msubsup><mml:mi>&#x03C3;</mml:mi><mml:mrow><mml:mi>S</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>t</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup><mml:mo>=</mml:mo><mml:mn>2</mml:mn><mml:mi>q</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>R</mml:mi><mml:mi>e</mml:mi><mml:mi>c</mml:mi><mml:mi>e</mml:mi><mml:mi>i</mml:mi><mml:mi>v</mml:mi><mml:mi>e</mml:mi><mml:mi>d</mml:mi></mml:mrow></mml:msub><mml:mo stretchy="false">)</mml:mo><mml:msup><mml:mi>M</mml:mi><mml:mrow><mml:mi>X</mml:mi><mml:mo>+</mml:mo><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mi>B</mml:mi><mml:mo>,</mml:mo></mml:math></disp-formula>where <inline-formula id="ieqn-54"><mml:math id="mml-ieqn-54"><mml:msub><mml:mi>K</mml:mi><mml:mrow><mml:mi>B</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is Boltzmann&#x2019;s constant, <inline-formula id="ieqn-55"><mml:math id="mml-ieqn-55"><mml:mi>T</mml:mi></mml:math></inline-formula> is absolute temperature, <inline-formula id="ieqn-56"><mml:math id="mml-ieqn-56"><mml:mi>B</mml:mi></mml:math></inline-formula> receiver bandwidth, and <inline-formula id="ieqn-57"><mml:math id="mml-ieqn-57"><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>L</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is equivalent load resistance [<xref ref-type="bibr" rid="ref-28">28</xref>,<xref ref-type="bibr" rid="ref-29">29</xref>]. Moreover, <inline-formula id="ieqn-58"><mml:math id="mml-ieqn-58"><mml:mi>q</mml:mi></mml:math></inline-formula> is the electron charge, <inline-formula id="ieqn-59"><mml:math id="mml-ieqn-59"><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> receiver sensitivity, and Bit error rate are then computed using [<xref ref-type="bibr" rid="ref-30">30</xref>,<xref ref-type="bibr" rid="ref-31">31</xref>]:
<disp-formula id="eqn-27"><label>(27)</label><mml:math id="mml-eqn-27" display="block"><mml:mi>B</mml:mi><mml:mi>E</mml:mi><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mi>Q</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:msqrt><mml:mi>S</mml:mi><mml:mi>N</mml:mi><mml:mi>R</mml:mi></mml:msqrt><mml:mo stretchy="false">)</mml:mo><mml:mo>,</mml:mo><mml:mi>Q</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>=</mml:mo><mml:mfrac><mml:mn>1</mml:mn><mml:msqrt><mml:mn>2</mml:mn><mml:mi>&#x03C0;</mml:mi></mml:msqrt></mml:mfrac><mml:msubsup><mml:mo>&#x222B;</mml:mo><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x221E;</mml:mi></mml:mrow></mml:mrow></mml:msubsup><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mfrac><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:msup><mml:mi>y</mml:mi><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mn>2</mml:mn></mml:mfrac></mml:mrow></mml:msup><mml:mi>d</mml:mi><mml:mi>y</mml:mi><mml:mo>.</mml:mo></mml:math></disp-formula></p>
<p>Furthermore, the factor (<inline-formula id="ieqn-60"><mml:math id="mml-ieqn-60"><mml:mi>Q</mml:mi></mml:math></inline-formula>) is calculated and used to estimate the performance of the receiver and its defined as follows [<xref ref-type="bibr" rid="ref-32">32</xref>]:
<disp-formula id="eqn-28"><label>(28)</label><mml:math id="mml-eqn-28" display="block"><mml:mi>Q</mml:mi><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mi>b</mml:mi><mml:mrow><mml:mi>o</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>b</mml:mi><mml:mrow><mml:mi>o</mml:mi><mml:mi>f</mml:mi><mml:mi>f</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:msub><mml:mi>&#x03C3;</mml:mi><mml:mrow><mml:mi>o</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:mfrac><mml:mo>,</mml:mo></mml:math></disp-formula></p>
<p>It accounts for the noise power variance when detecting 1 and 0 bits. Another key parameter is the link margin, which evaluates the link&#x2019;s ability to compensate for scintillation, scattering, and absorption losses. The link margin is defined by [<xref ref-type="bibr" rid="ref-33">33</xref>]:
<disp-formula id="eqn-29"><label>(29)</label><mml:math id="mml-eqn-29" display="block"><mml:mi>L</mml:mi><mml:mi>M</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>T</mml:mi><mml:mi>o</mml:mi><mml:mi>t</mml:mi><mml:mi>a</mml:mi><mml:mi>l</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mrow><mml:mo>|</mml:mo><mml:msub><mml:mi>S</mml:mi><mml:mrow><mml:mi>r</mml:mi></mml:mrow></mml:msub><mml:mo>|</mml:mo></mml:mrow><mml:mo>+</mml:mo><mml:msub><mml:mi>G</mml:mi><mml:mrow><mml:mi>R</mml:mi></mml:mrow></mml:msub><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>G</mml:mi><mml:mi>e</mml:mi><mml:mi>o</mml:mi><mml:mi>m</mml:mi><mml:mi>e</mml:mi><mml:mi>t</mml:mi><mml:mi>r</mml:mi><mml:mi>i</mml:mi><mml:mi>c</mml:mi><mml:mi>a</mml:mi><mml:mi>l</mml:mi></mml:mrow></mml:msub><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>T</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>R</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>A</mml:mi><mml:mi>t</mml:mi><mml:mi>m</mml:mi><mml:mi>o</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi><mml:mi>h</mml:mi><mml:mi>e</mml:mi><mml:mi>r</mml:mi><mml:mi>i</mml:mi><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>.</mml:mo></mml:math></disp-formula></p>
<p>Total transmitted power <inline-formula id="ieqn-61"><mml:math id="mml-ieqn-61"><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>T</mml:mi><mml:mi>t</mml:mi><mml:mi>o</mml:mi><mml:mi>t</mml:mi><mml:mi>a</mml:mi><mml:mi>l</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>, receiver sensitivity <inline-formula id="ieqn-62"><mml:math id="mml-ieqn-62"><mml:msub><mml:mi>S</mml:mi><mml:mrow><mml:mi>r</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>, and receiver gain <inline-formula id="ieqn-63"><mml:math id="mml-ieqn-63"><mml:msub><mml:mi>G</mml:mi><mml:mrow><mml:mi>R</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> are key factors in this equation. Additionally, the parameters <inline-formula id="ieqn-64"><mml:math id="mml-ieqn-64"><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>G</mml:mi><mml:mi>e</mml:mi><mml:mi>o</mml:mi><mml:mi>m</mml:mi><mml:mi>e</mml:mi><mml:mi>t</mml:mi><mml:mi>r</mml:mi><mml:mi>i</mml:mi><mml:mi>c</mml:mi><mml:mi>a</mml:mi><mml:mi>l</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>, <inline-formula id="ieqn-65"><mml:math id="mml-ieqn-65"><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>T</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>, <inline-formula id="ieqn-66"><mml:math id="mml-ieqn-66"><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>R</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> and <inline-formula id="ieqn-67"><mml:math id="mml-ieqn-67"><mml:msub><mml:mi>L</mml:mi><mml:mrow><mml:mi>A</mml:mi><mml:mi>t</mml:mi><mml:mi>m</mml:mi><mml:mi>o</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi><mml:mi>h</mml:mi><mml:mi>e</mml:mi><mml:mi>r</mml:mi><mml:mi>i</mml:mi><mml:mi>c</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> are considered, representing geometrical, transmitter-receiver, and atmospheric losses. It&#x2019;s assumed that scintillation losses due to high-speed train travel are neglected. To determine the required number of BSs for continuous coverage along the rail track, the calculation is as follows:
<disp-formula id="eqn-30"><label>(30)</label><mml:math id="mml-eqn-30" display="block"><mml:mi>N</mml:mi><mml:mo>.</mml:mo><mml:msub><mml:mi>B</mml:mi><mml:mrow><mml:mrow><mml:mo>/</mml:mo></mml:mrow><mml:mn>1</mml:mn><mml:mi>k</mml:mi><mml:mi>m</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1000</mml:mn><mml:mi>m</mml:mi></mml:mrow><mml:mrow><mml:mi>M</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mi>i</mml:mi><mml:mi>m</mml:mi><mml:mi>u</mml:mi><mml:mi>m</mml:mi><mml:mtext>&#x00A0;</mml:mtext><mml:mi>A</mml:mi><mml:mi>c</mml:mi><mml:mi>c</mml:mi><mml:mi>e</mml:mi><mml:mi>p</mml:mi><mml:mi>t</mml:mi><mml:mi>a</mml:mi><mml:mi>b</mml:mi><mml:mi>l</mml:mi><mml:mi>e</mml:mi><mml:mtext>&#x00A0;</mml:mtext><mml:mi>L</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>k</mml:mi><mml:mtext>&#x00A0;</mml:mtext><mml:mi>R</mml:mi><mml:mi>a</mml:mi><mml:mi>n</mml:mi><mml:mi>g</mml:mi><mml:mi>e</mml:mi></mml:mrow></mml:mfrac><mml:mo>,</mml:mo></mml:math></disp-formula>where acceptable link range is governed by an error-free FSO link with BER of 10<sup>&#x2212;9</sup>. <xref ref-type="disp-formula" rid="eqn-6">Eq. (6)</xref> is used for 1 km rail track and <xref ref-type="disp-formula" rid="eqn-7">Eq. (7)</xref> for a 10 km rail track.
<disp-formula id="eqn-31"><label>(31)</label><mml:math id="mml-eqn-31" display="block"><mml:mi>N</mml:mi><mml:mo>.</mml:mo><mml:msub><mml:mi>B</mml:mi><mml:mrow><mml:mrow><mml:mo>/</mml:mo></mml:mrow><mml:mn>10</mml:mn><mml:mi>k</mml:mi><mml:mi>m</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>10</mml:mn><mml:mo>,</mml:mo><mml:mspace width="negativethinmathspace" /><mml:mn>000</mml:mn><mml:mi>m</mml:mi></mml:mrow><mml:mrow><mml:mi>M</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mi>i</mml:mi><mml:mi>m</mml:mi><mml:mi>u</mml:mi><mml:mi>m</mml:mi><mml:mtext>&#x00A0;</mml:mtext><mml:mi>A</mml:mi><mml:mi>c</mml:mi><mml:mi>c</mml:mi><mml:mi>e</mml:mi><mml:mi>p</mml:mi><mml:mi>t</mml:mi><mml:mi>a</mml:mi><mml:mi>b</mml:mi><mml:mi>l</mml:mi><mml:mi>e</mml:mi><mml:mtext>&#x00A0;</mml:mtext><mml:mi>L</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>k</mml:mi><mml:mtext>&#x00A0;</mml:mtext><mml:mi>R</mml:mi><mml:mi>a</mml:mi><mml:mi>n</mml:mi><mml:mi>g</mml:mi><mml:mi>e</mml:mi></mml:mrow></mml:mfrac><mml:mo>.</mml:mo></mml:math></disp-formula></p>
</sec>
<sec id="s2_6">
<label>2.6</label>
<title>Channel Model</title>
<p>FSO link establishes an optical link using the earth&#x2019;s atmosphere. This limits beam transmission due to photon absorption and scattering. Fog and rain attenuation levels were assessed using meteorological data and empirical models. Rain and fog attenuations were categorized by ITU-R code to characterize FSO channel [<xref ref-type="bibr" rid="ref-34">34</xref>]. <xref ref-type="table" rid="table-1">Table 1</xref> presents the link power budget for the curved track FSO-G2T communication link used in this simulation, with a wavelength of 1550 nm and a data rate of 2.5 Gbps.</p>
<table-wrap id="table-1">
<label>Table 1</label>
<caption>
<title>Link power budget for FSO-G2T OOK-NRZ on curved track</title>
</caption>
<table frame="hsides">
<colgroup>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
</colgroup>
<thead>
<tr>
<th align="center" colspan="6">Transmitter parameters</th>
</tr>
<tr>
<th>Parameters</th>
<th>Unit</th>
<th align="center" colspan="4">Value</th>
</tr>
</thead>
<tbody>
<tr>
<td>Peak laser power</td>
<td><bold>mW</bold></td>
<td align="center" colspan="4">20</td>
</tr>
<tr>
<td>Wavelength (&#x03BB;)</td>
<td><bold>nm</bold></td>
<td align="center" colspan="4">1550</td>
</tr>
<tr>
<td>Data rate (Br)</td>
<td><bold>Gbps</bold></td>
<td align="center" colspan="4">2.5</td>
</tr>
<tr>
<td>Transmitter aperture diameter (d<sub>T</sub>)</td>
<td><bold>Cm</bold></td>
<td align="center" colspan="4">8</td>
</tr>
<tr>
<td>Modulation format</td>
<td><bold>&#x2013;</bold></td>
<td align="center" colspan="4"><bold>OOK-NRZ</bold></td>
</tr>
<tr>
<td>Transmitted power (P<sub>T</sub>)</td>
<td><bold>dBm</bold></td>
<td>16.19</td>
<td>14.94</td>
<td>13.18</td>
<td>10.17</td>
</tr>
<tr>
<td>Transmitter system loss (L<sub>Tx</sub>)</td>
<td><bold>dB</bold></td>
<td>&#x2212;1.5</td>
<td>&#x2212;1.5</td>
<td>&#x2212;1.5</td>
<td>&#x2212;1.5</td>
</tr>
<tr>
<td>Number of transmitters (N<sub>TX</sub>)</td>
<td><bold>Unit(s)</bold></td>
<td>4</td>
<td>3</td>
<td>2</td>
<td>1</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>The G2T-FSO communication system, shown in <xref ref-type="fig" rid="fig-5">Fig. 5</xref>, was modeled in OptiSystem with a 4Tx-1Rx configuration. It uses multiple lasers connected to a single OOK modulator to produce multiple beams that propagate along the link.</p>
<fig id="fig-5">
<label>Figure 5</label>
<caption>
<title>Example of 4Tx/1Rx G2T-FSO transmitters</title>
</caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="CMES_55679-fig-5.tif"/>
</fig>
<sec id="s2_6_1">
<label>2.6.1</label>
<title>Rain Attenuation</title>
<p>The model proposed by Carbonneau is frequently employed in the estimation of rain attenuation, utilizing the rain rate <italic>R</italic> (mm/h). The model incorporates two constants, and <italic>k</italic>, which are dependent on the specific measured values. The variable &#x03B3;<sub><italic>Rain</italic></sub> represents the rain attenuation per km and is defined as:
<disp-formula id="eqn-32"><label>(32)</label><mml:math id="mml-eqn-32" display="block"><mml:msub><mml:mi>&#x03B3;</mml:mi><mml:mrow><mml:mi>R</mml:mi><mml:mi>a</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mi>k</mml:mi><mml:mo>.</mml:mo><mml:mi>R</mml:mi><mml:mi>&#x03B1;</mml:mi><mml:mo stretchy="false">[</mml:mo><mml:mi>m</mml:mi><mml:mi>m</mml:mi><mml:mrow><mml:mo>/</mml:mo></mml:mrow><mml:mi>h</mml:mi><mml:mi>r</mml:mi><mml:mo stretchy="false">]</mml:mo><mml:mo>.</mml:mo></mml:math></disp-formula></p>
</sec>
<sec id="s2_6_2">
<label>2.6.2</label>
<title>Fog Attenuation</title>
<p>Ensuring a clear LOS between transceivers is crucial for the proper functioning of the FSO link. Therefore, a visible path is required. Fog particles play a crucial role in the absorption of photons in the Earth&#x2019;s atmosphere. Their small size, which is comparable to the wavelength transmission window [<xref ref-type="bibr" rid="ref-35">35</xref>], makes them a significant factor. Fog can considerably impact link transparency, resulting in a reduced LOS range. The attenuation caused by fog can be as high as 300 dB/km, making it a key consideration in FSO link design. One common approach to estimating fog attenuation is through Mie scattering theory, which relies on measurements of atmospheric transparency, often referred to as visibility [<xref ref-type="bibr" rid="ref-34">34</xref>&#x2013;<xref ref-type="bibr" rid="ref-36">36</xref>]. Fog attenuation is computed as follows:
<disp-formula id="eqn-33"><label>(33)</label><mml:math id="mml-eqn-33" display="block"><mml:msub><mml:mi>&#x03B1;</mml:mi><mml:mrow><mml:mi>F</mml:mi><mml:mi>o</mml:mi><mml:mi>g</mml:mi><mml:mo stretchy="false">[</mml:mo><mml:mi>d</mml:mi><mml:mi>B</mml:mi><mml:mrow><mml:mo>/</mml:mo></mml:mrow><mml:mi>K</mml:mi><mml:mi>m</mml:mi><mml:mo stretchy="false">]</mml:mo></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mn>3.91</mml:mn><mml:msub><mml:mi>V</mml:mi><mml:mrow><mml:mi>k</mml:mi><mml:mi>m</mml:mi></mml:mrow></mml:msub></mml:mfrac><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mfrac><mml:msub><mml:mi>&#x03BB;</mml:mi><mml:mrow><mml:mi>n</mml:mi><mml:mi>m</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mn>550</mml:mn><mml:mrow><mml:mi>n</mml:mi><mml:mi>m</mml:mi></mml:mrow></mml:msub></mml:mfrac><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mi>q</mml:mi></mml:mrow></mml:msup><mml:mo>.</mml:mo></mml:math></disp-formula>where <italic>V</italic> represents visibility in km, &#x03BB;<sub><italic>nm</italic></sub> denotes wavelength in nm and &#x003B1; is the fog attenuation factor in dB/Km. The scattering size distribution, <italic>q</italic>, as defined by KIM [<xref ref-type="bibr" rid="ref-34">34</xref>], is illustrated in <xref ref-type="disp-formula" rid="eqn-34">(34)</xref>. An attenuation coefficient of 0.6 dB/km was adopted to characterize clear weather conditions, with other geometrical parameters listed in <xref ref-type="table" rid="table-2">Table 2</xref>.</p>
<table-wrap id="table-2">
<label>Table 2</label>
<caption>
<title>Curved track G2T-FSO geometrical parameters</title>
</caption>
<table frame="hsides">
<colgroup>
<col align="left"/>
<col align="left"/>
<col align="left"/>
</colgroup>
<thead>
<tr>
<th>Parameter</th>
<th>Symbol</th>
<th>Value</th>
</tr>
</thead>
<tbody>
<tr>
<td>Tilt angle</td>
<td><italic>&#x03B3;</italic></td>
<td>2.25&#x00B0;</td>
</tr>
<tr>
<td>Coverage angle</td>
<td><italic>&#x03B4;</italic></td>
<td>0.65&#x00B0;</td>
</tr>
<tr>
<td>Receiver FOV</td>
<td><italic>&#x03C6;</italic></td>
<td>5.15</td>
</tr>
<tr>
<td>Track vertical distance</td>
<td><inline-formula id="ieqn-68"><mml:math id="mml-ieqn-68"><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>V</mml:mi><mml:mi>C</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula></td>
<td>5&#x2013;25 m</td>
</tr>
<tr>
<td>Track horizontal distance</td>
<td><inline-formula id="ieqn-69"><mml:math id="mml-ieqn-69"><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>H</mml:mi><mml:mi>C</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula></td>
<td>1&#x2013;2 m</td>
</tr>
<tr>
<td>Track coverage distance</td>
<td><italic>L</italic><sub><italic>C</italic></sub></td>
<td>1 km</td>
</tr>
<tr>
<td>Curved track link range</td>
<td><italic>Z</italic><sub><italic>C</italic></sub></td>
<td>0&#x2013;1000 m</td>
</tr>
<tr>
<td>Curved tracks clearance</td>
<td><italic>CL</italic></td>
<td>5 m</td>
</tr>
<tr>
<td>Track radius at V &#x003D; 250 km/h</td>
<td>R<sub>C</sub> (250)</td>
<td>2667 m</td>
</tr>
<tr>
<td>Divergence angle for track RC (250)</td>
<td><italic>&#x03B8;</italic><sub>C</sub></td>
<td>0&#x2013;1.5&#x00B0;</td>
</tr>
</tbody>
</table>
</table-wrap>
<p><disp-formula id="eqn-34"><label>(34)</label><mml:math id="mml-eqn-34" display="block"><mml:mi>q</mml:mi><mml:mo>=</mml:mo><mml:mrow><mml:mo>{</mml:mo><mml:mtable columnalign="left left" rowspacing=".2em" columnspacing="1em" displaystyle="false"><mml:mtr><mml:mtd /><mml:mtd><mml:mn>1.6</mml:mn></mml:mtd></mml:mtr><mml:mtr><mml:mtd /><mml:mtd><mml:mn>1.3</mml:mn></mml:mtd></mml:mtr><mml:mtr><mml:mtd /><mml:mtd><mml:mn>0.16</mml:mn><mml:mi>V</mml:mi><mml:mo>+</mml:mo><mml:mn>1.34</mml:mn></mml:mtd></mml:mtr><mml:mtr><mml:mtd /><mml:mtd><mml:mi>V</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>0.5</mml:mn></mml:mtd></mml:mtr><mml:mtr><mml:mtd /><mml:mtd><mml:mn>0</mml:mn></mml:mtd></mml:mtr></mml:mtable><mml:mo fence="true" stretchy="true" symmetric="true"></mml:mo></mml:mrow><mml:mtable rowspacing="4pt" columnspacing="1em"><mml:mtr><mml:mtd><mml:mi>f</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mi>f</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mi>f</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mi>f</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mi>f</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi></mml:mtd></mml:mtr></mml:mtable><mml:mtable rowspacing="4pt" columnspacing="1em"><mml:mtr><mml:mtd><mml:mi>H</mml:mi><mml:mi>i</mml:mi><mml:mi>g</mml:mi><mml:mi>h</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mspace width="thinmathspace" /><mml:mi>A</mml:mi><mml:mi>v</mml:mi><mml:mi>e</mml:mi><mml:mi>r</mml:mi><mml:mi>a</mml:mi><mml:mi>g</mml:mi><mml:mi>e</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mi>H</mml:mi><mml:mi>a</mml:mi><mml:mi>z</mml:mi><mml:mi>e</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mi>M</mml:mi><mml:mi>i</mml:mi><mml:mi>s</mml:mi><mml:mi>t</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mi>F</mml:mi><mml:mi>o</mml:mi><mml:mi>g</mml:mi></mml:mtd></mml:mtr></mml:mtable><mml:mtable rowspacing="4pt" columnspacing="1em"><mml:mtr><mml:mtd><mml:mi>V</mml:mi><mml:mi>i</mml:mi><mml:mi>s</mml:mi><mml:mi>i</mml:mi><mml:mi>b</mml:mi><mml:mi>i</mml:mi><mml:mi>l</mml:mi><mml:mi>i</mml:mi><mml:mi>t</mml:mi><mml:mi>y</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mspace width="thinmathspace" /><mml:mi>V</mml:mi><mml:mi>i</mml:mi><mml:mi>s</mml:mi><mml:mi>i</mml:mi><mml:mi>b</mml:mi><mml:mi>i</mml:mi><mml:mi>l</mml:mi><mml:mi>i</mml:mi><mml:mi>t</mml:mi><mml:mi>y</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mi>V</mml:mi><mml:mi>i</mml:mi><mml:mi>s</mml:mi><mml:mi>i</mml:mi><mml:mi>b</mml:mi><mml:mi>i</mml:mi><mml:mi>l</mml:mi><mml:mi>i</mml:mi><mml:mi>t</mml:mi><mml:mi>y</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mi>V</mml:mi><mml:mi>i</mml:mi><mml:mi>s</mml:mi><mml:mi>i</mml:mi><mml:mi>b</mml:mi><mml:mi>i</mml:mi><mml:mi>l</mml:mi><mml:mi>i</mml:mi><mml:mi>t</mml:mi><mml:mi>y</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mi>V</mml:mi><mml:mi>i</mml:mi><mml:mi>s</mml:mi><mml:mi>i</mml:mi><mml:mi>b</mml:mi><mml:mi>i</mml:mi><mml:mi>l</mml:mi><mml:mi>i</mml:mi><mml:mi>t</mml:mi><mml:mi>y</mml:mi></mml:mtd></mml:mtr></mml:mtable><mml:mtable rowspacing="4pt" columnspacing="1em"><mml:mtr><mml:mtd><mml:mi>V</mml:mi><mml:mo>&#x003E;</mml:mo><mml:mn>50</mml:mn><mml:mi>k</mml:mi><mml:mi>m</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mspace width="1em" /><mml:mn>6</mml:mn><mml:mi>k</mml:mi><mml:mi>m</mml:mi><mml:mo>&#x003C;</mml:mo><mml:mi>V</mml:mi><mml:mo>&#x003C;</mml:mo><mml:mn>50</mml:mn><mml:mi>k</mml:mi><mml:mi>m</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mspace width="1em" /><mml:mn>1</mml:mn><mml:mi>k</mml:mi><mml:mi>m</mml:mi><mml:mo>&#x003C;</mml:mo><mml:mi>V</mml:mi><mml:mo>&#x003C;</mml:mo><mml:mn>6</mml:mn><mml:mi>k</mml:mi><mml:mi>m</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mspace width="1em" /><mml:mn>0.5</mml:mn><mml:mi>k</mml:mi><mml:mi>m</mml:mi><mml:mo>&#x003C;</mml:mo><mml:mi>V</mml:mi><mml:mo>&#x003C;</mml:mo><mml:mn>1</mml:mn><mml:mi>k</mml:mi><mml:mi>m</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mi>V</mml:mi><mml:mo>&#x003C;</mml:mo><mml:mn>0.5</mml:mn><mml:mi>k</mml:mi><mml:mi>m</mml:mi></mml:mtd></mml:mtr></mml:mtable><mml:mtext>&#x00A0;&#x00A0;&#x00A0;</mml:mtext><mml:mo>.</mml:mo></mml:math></disp-formula></p>
</sec>
</sec>
</sec>
<sec id="s3">
<label>3</label>
<title>Results Discussion</title>
<p>This section presents the performance evaluation of G2T-FSO communication link in terms of received power, SNR, BER, and eye diagram.</p>
<sec id="s3_1">
<label>3.1</label>
<title>Received Power and SNR</title>
<p><xref ref-type="fig" rid="fig-6">Fig. 6</xref> illustrates received power levels for curved track G2T-FSO communication link with a radius of R<sub>C1(250)</sub> &#x003D; 2667 m. It shows the effects of different weather conditions on received power levels along the track span.</p>
<fig id="fig-6">
<label>Figure 6</label>
<caption>
<title>G2T-FSO received power for curved track link with NRZ modulation: (a) 1Tx/1Rx, (b) 2Tx/1Rx, (c) 3Tx/1Rx, (d) 4Tx/1Rx</title>
</caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="CMES_55679-fig-6.tif"/>
</fig>
<p>Moreover, it is divided into two regions, namely, feasible region and infeasible region. The feasible region shows levels for acceptable link performance that achieved a BER of 10<sup>&#x2212;9</sup>, however, the infeasible region shows power levels that are less than the acceptable levels.</p>
<p>In terms of link G2T-FSO range, under clear weather with attenuation of 0.6 dB/km power levels of &#x2212;29.71, &#x2212;29.05 and &#x2212;29.50 dBm were achieved at ranges of 240, 365, 505, and 618 m for 1Tx, 2Tx, 3Tx, and 4Tx NRZ transmitter respectively. Furthermore, under moderate rain attenuation of 6.9 dB/km levels of &#x2212;28.68, &#x2212;29.50, &#x2212;29.73 and &#x2212;28.99 dBm at ranges of 201, 322, 388 and 399 m for single, dual, triple and quad transmitters, respectively, Moreover, under moderate fog levels of &#x2212;29.32, &#x2212;28.83, &#x2212;28.56 and &#x2212;29.10 dBm at ranges of 164, 220,260 and 301 m for the aforementioned cases, respectively.</p>
<p>On the other hand, in terms of weather effects on received power, under moderate rain, an average decline of &#x2212;5.15 and &#x2212;3.07 dBm occurred for 4Tx and 3Tx, 2Tx, 1Tx, respectively, which is equivalent to an average drop of 22%, 10.36%, 13% and 7.59% for each case, respectively. Furthermore, moderate fog causes an average power level decrease of &#x2212;13.74, &#x2212;13.74, &#x2212;13.79 and &#x2212;13.81 dBm that amounting to an average of 43.84%, 38.92%, 38.34% and 29.67% for 4Tx, 3Tx, 2Tx and 1Tx, respectively. The Quad Transmitter setup achieved the highest link range and robust performance in various weather conditions. The train communicates through all four transceivers (Tx1, Tx2, Tx3, Tx4) with the BS Transceiver (Rx1), enabling high data rates for passengers.</p>
<p>Acquired SNR levels of multiple receivers under variable weather conditions are illustrated in <xref ref-type="fig" rid="fig-7">Fig. 7</xref>. It is organized into four subgroups (a), (b), (c) and (d) for single, dual, Triple, and Quad transmitters, respectively. In the case of clear weather conditions, SNR levels of 4.06, 5.39, 4.43 and 4.47 dB at ranges of 240, 265, 505, and 618 m were achieved for the cases above, respectively. Moreover, under moderate rain conditions, levels of 5.66, 4.31, 7.64, and 6.40 dB were achieved at link ranges of 201, 322, 388, and 399 m for 1Tx, 2Tx, 3Tx, and 4Tx, respectively. Lastly, under moderate fog condition SNR levels of 4.73, 6.28, 6.45, and 5.24 dB were achieved at ranges of 164, 220, 260, and 301 m.</p>
<fig id="fig-7">
<label>Figure 7</label>
<caption>
<title>G2T-FSO curved track link SNR for NRZ modulation: (a) 1Tx/1Rx, (b) 2Tx/1Rx, (c) 3Tx/1Rx, (d) 4Tx/1Rx</title>
</caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="CMES_55679-fig-7.tif"/>
</fig>
<p>As per international Union of Railways (UIC) standards for high-speed railways, the train-to-train communication model achieves optimal performance with a BER &#x003D; 10<sup>&#x2212;9</sup> at an SNR of 5 dB or higher, meeting transmission needs for train control and prewarning messages. Simulations show that the 4Tx/1Rx configuration provides the highest SNR as the train nears the BS.</p>
</sec>
<sec id="s3_2">
<label>3.2</label>
<title>BER and Eye Diagrams</title>
<p><xref ref-type="fig" rid="fig-8">Fig. 8</xref> shows achieved BER levels along with coverage range for a various number of G2T-FSO curved Track transmitters under different weather conditions. The BER is a key parameter for evaluating the performance of data channels, whether over radio, wireless, or wired telecommunications links. It measures the number of errors occurring in the transmitted data, with an acceptable BER typically around 10<sup>&#x2212;9</sup>, indicating very low error rates at the receiving end. The graphs demonstrate acceptable BER levels of 10<sup>&#x2212;9</sup> were achievable at ranges of 240, 365, 505 and 610 m for 1Tx, 2Tx, 3Tx, and 4Tx, respectively. Additionally, under moderate rain condition, acceptable link performance was achieved at 201, 322, 388, and 399 m. Apart from rain attenuation, moderate fog acceptable link ranges were achieved at distances of 164, 220, 260 and 301 m for 1Tx, 2Tx, 3Tx, and 4Tx, respectively.</p>
<fig id="fig-8">
<label>Figure 8</label>
<caption>
<title>G2T-FSO curved track link BER for NRZ modulation: (a) 1Tx/1Rx, (b) 2Tx/1Rx, (c) 3Tx/1Rx, (d) 4Tx/1Rx</title>
</caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="CMES_55679-fig-8.tif"/>
</fig>
<p>An eye diagram, used to assess signal quality, appears as a series of &#x201C;eyes&#x201D; between rails. <xref ref-type="table" rid="table-3">Table 3</xref> shows that the 4Tx configuration performs best under clear, moderate rain, and moderate fog conditions. All transmitter configurations show near-ideal NRZ eye openings at short distances, but eye clarity decreases with greater distance or higher weather attenuation. Moderate fog degrades performance, leading to incoherent eye diagrams at long ranges. The 4Tx configuration exhibits high tolerance to geometrical losses in clear weather but some jitter in moderate rain. The 3Tx configuration also handles weather well but is less effective than 4Tx in moderate fog.</p>
<table-wrap id="table-3">
<label>Table 3</label>
<caption>
<title>Eye diagrams and their relationships for G2T-FSO curved track link</title>
</caption>
<table frame="hsides">
<colgroup>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
</colgroup>
<thead>
<tr>
<td></td>
<td></td>
<td></td>
<td></td>
<td></td>
<td></td>
<td></td>
<td></td>
<td></td>
<td></td>
</tr>
</thead>
<tbody>
<tr>
<td>Weather</td>
<td align="center" colspan="3">Clear</td>
<td align="center" colspan="3">Moderate rain</td>
<td align="center" colspan="3">Moderate fog</td>
</tr>
<tr>
<td>Link range (m)</td>
<td>164</td>
<td>365</td>
<td>580</td>
<td>164</td>
<td>365</td>
<td>580</td>
<td>164</td>
<td>365</td>
<td>580</td>
</tr>
<tr>
<td>Divergence (mrad)</td>
<td>11.63</td>
<td>17.5</td>
<td>21.05</td>
<td>11.63</td>
<td>17.5</td>
<td>21.05</td>
<td>11.63</td>
<td>17.5</td>
<td>21.05</td>
</tr>
<tr>
<td>Attenuation (dB/km)</td>
<td align="center" colspan="3">&#x2212;0.6</td>
<td align="center" colspan="3">&#x2212;6.9</td>
<td align="center" colspan="3">&#x2212;28.9</td>
</tr>
<tr>
<td>Geometrical loss (dB)</td>
<td>&#x2212;31.98</td>
<td>&#x2212;42.25</td>
<td>&#x2212;47.82</td>
<td>&#x2212;31.98</td>
<td>&#x2212;42.25</td>
<td>&#x2212;47.82</td>
<td>&#x2212;31.98</td>
<td>&#x2212;42.25</td>
<td>&#x2212;47.82</td>
</tr>
<tr>
<td>Train position</td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-1.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-2.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-3.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-4.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-5.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-6.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-7.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-8.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-9.tif"/></p></td>
</tr>
<tr>
<td>Eye diagram for 1Tx/1Rx 10.39 dBm</td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-10.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-11.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-12.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-13.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-14.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-15.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-16.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-17.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-18.tif"/></p></td>
</tr>
<tr>
<td>Eye diagram for 2Tx/1Rx 20.55 dBm</td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-19.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-20.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-21.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-22.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-23.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-24.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-25.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-26.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-27.tif"/></p></td>
</tr>
<tr>
<td>Eye diagram 55 For 3Tx/1Rx 31.78 dBm</td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-28.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-29.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-30.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-31.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-32.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-33.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-34.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-35.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-36.tif"/></p></td>
</tr>
<tr>
<td>Eye diagram for 4Tx/1Rx 41.50 dBm</td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-37.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-38.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-39.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-40.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-41.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-42.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-43.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-44.tif"/></p></td>
<td><p><inline-graphic xlink:href="CMES_55679-inline-45.tif"/></p></td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s3_3">
<label>3.3</label>
<title>Link Margin Analysis for Curve Track</title>
<p>A curved track with a radius of R<sub>C1(250)</sub> &#x003D; 2667 m for link margin analysis in <xref ref-type="fig" rid="fig-9">Fig. 9</xref>, shows resulted link margins for curved track model were estimated where it illustrates link margins for NRZ for 4Tx, 3Tx, 2Tx and 1Tx under various weather conditions. However, under clear weather link margins of 21, 22.16, 24.32 and 26.59 dB were achieved at ranges of 618, 505, 365, and 240 m for 4Tx, 3Tx, 2Tx and 1Tx utilizing NRZ modulated transmitters. This result shows how track curvature impacts FSO link stability.</p>
<fig id="fig-9">
<label>Figure 9</label>
<caption>
<title>Link margins analysis NRZ transmitters for curved track G2T-FSO model</title>
</caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="CMES_55679-fig-9.tif"/>
</fig>
</sec>
<sec id="s3_4">
<label>3.4</label>
<title>Comparison of Curved Track G2T-FSO Model Related Research</title>
<p>For the case of curved track G2T-FSO line, there is only one study that has been conducted by Paudel et al. in [<xref ref-type="bibr" rid="ref-8">8</xref>]. <xref ref-type="table" rid="table-4">Table 4</xref> shows that 4TX/1RXNRZ G2T-FSO link achieve 124% improvements, respectively.</p>
<table-wrap id="table-4">
<label>Table 4</label>
<caption>
<title>Comparison of related research</title>
</caption>
<table frame="hsides">
<colgroup>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
</colgroup>
<thead>
<tr>
<th>No.</th>
<th>Reference</th>
<th>Maximum coverage range</th>
<th>Difference (m)</th>
</tr>
</thead>
<tbody>
<tr>
<td>1.</td>
<td>Paudel et al. [<xref ref-type="bibr" rid="ref-8">8</xref>]</td>
<td>145</td>
<td>&#x2013;</td>
</tr>
<tr>
<td><bold>2.</bold></td>
<td><bold>4TX/1RX NRZ</bold></td>
<td>618</td>
<td>473</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
</sec>
<sec id="s4">
<label>4</label>
<title>Conclusions</title>
<p>This research paper studies the received power, SNR, BER, and eye diagrams for the G2T-FSO link for the curved track. A number of fundamental G2T-FSO link geometrical and mathematical properties were derived and defined in terms of received power and SNR. The simulation was set up to evaluate the performance of the curved track model based on multiple transmitters (1Tx/1Rx, 2Tx/1Rx, 3Tx/1Rx and 4Tx/1Rx), NRZ-OOK modulation, and different weather conditions. This research paper also provides detailed formulations for the curved track G2T-FSO model and a summary of the respective link range, attenuation, received power, and eye diagrams tabulated as in <xref ref-type="table" rid="table-3">Table 3</xref>. In comparison with related work, this proposed curve G2T-FSO model link illustrated improved performance and longer coverage ranges. Although the proposed FSO technology poses many advantages there are limitations, where severe weather conditions have the potential to limit link availability, performance, and range. Therefore, based on the results, it was observed that in order to establish an acceptable link performance with the least number of base stations, increasing the number of transmitters is preferred.</p>

</sec>
</body>
<back>
<ack>
<p>The authors extend their appreciation to the Deputyship for Research &#x0026; Innovation, Ministry of Education in Saudi Arabia for funding this research work through the project.</p>
</ack>
<sec><title>Funding Statement</title>
<p>This research was funded by the Deputyship for Research &#x0026; Innovation, Ministry of Education in Saudi Arabia, grant number S-1443-0223.</p>
</sec>
<sec><title>Author Contributions</title>
<p>The authors confirm contribution to the paper as follows: Conceptualization, Wafi A. B. Mabrouk, Mohammed A. Alhartomi, Mohammad F. L. Abdullah and Ahmed Alzahmi; methodology, Mohammed A. Alhartomi, Mohammad F. L. Abdullah, Wafi A. B. Mabrouk and Mohammed S. M. Gismalla; software, Wafi A. B. Mabrouk and Mohammed S. M. Gismalla; validation, Mohammad F. L. Abdullah, Wafi A. B. Mabrouk and Mohammed S. M. Gismalla; formal analysis, Wafi A. B. Mabrouk and Mohammed S. M. Gismalla; investigation, Mohammed A. Alhartomi, Ahmed Alzahmi, Saeed Alzahrani and Mohammad R. Altimania; resources, Ahmed Alzahmi, Saeed Alzahrani, Mohammad R. Altimania and Mohammed S. Alsawat; data curation, Ahmed Alzahmi, Saeed Alzahrani, Mohammad R. Altimania and Mohammed S. Alsawat; writing&#x2014;original draft preparation, Wafi A. B. Mabrouk, Mohammad F. L. Abdullah and Mohammed A. Alhartomi; writing&#x2014;review and editing, Mohammed S. M. Gismalla, Mohammed A. Alhartomi and Mohammad F. L. Abdullah; visualization, Wafi A. B. Mabrouk, Ahmed Alzahmi and Mohammed A. Alhartomi; supervision, Mohammed A. Alhartomi and Mohammad F. L. Abdullah; project administration, Ahmed Alzahmi and Mohammed A. Alhartomi; funding acquisition, Mohammed A. Alhartomi, Ahmed Alzahmi, Saeed Alzahrani, Mohammad R. Altimania and Mohammed S. Alsawat. All authors reviewed the results and approved the final version of the manuscript.</p>
</sec>
<sec sec-type="data-availability"><title>Availability of Data and Materials</title>
<p>The data that support the findings of this study are available on request from the corresponding author.</p>
</sec>
<sec><title>Ethics Approval</title>
<p>Not applicable.</p>
</sec>
<sec sec-type="COI-statement"><title>Conflicts of Interest</title>
<p>The authors declare that they have no conflicts of interest to report regarding the present study.</p>
</sec>
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